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The layer potential technique for the inverse conductivity problem. (English) Zbl 0857.35134

Summary: We consider the inverse conductivity problem for the equation \[ \text{div} ((1+(k-1)\chi_D)\nabla u)=0 \] determining the unknown object \(D\) contained in a domain \(\Omega\) with one measurement on \(\partial\Omega\). The method in this paper is the layer potential technique. We find a representation formula for the solution to the equation using single layer potentials on \(D\) and \(\Omega\). Using this representation formula, we prove that the location and size of a disk \(D\) contained in a simply connected bounded Lipschitz domain \(\Omega\) can be determined with one measurement corresponding to arbitrary non-zero Neumann data on \(\partial\Omega\). (Previously, it was known that a disk can be determined with one measurement if \(\Omega\) is assumed to be the half space.) We also prove a weaker version of the uniqueness for balls in \(\mathbb{R}^n\) \((n\geq 3)\) with one measurement corresponding to a certain Neumann data.

MSC:

35R30 Inverse problems for PDEs
35J25 Boundary value problems for second-order elliptic equations
31B10 Integral representations, integral operators, integral equations methods in higher dimensions
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